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A Selective Modern History of the Boltzmann and Related Equations Reinhard Illner, Victoria October 2014, Fields Institute Reinhard Illner, Victoria A Selective Modern History of the Boltzmann and Related Equati Synopsis 1. I have


  1. A Selective “Modern” History of the Boltzmann and Related Equations Reinhard Illner, Victoria October 2014, Fields Institute Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  2. Synopsis 1. I have an ambivalent relation to surveys! 2. Key Words, Tools, People 3. Powerful Tools, I: Potentials for Interaction 4. An entertaining digression: The Digits of Π 5. Powerful Tools, II: Velocity Averaging 6. Powerful Tools, III: Functionals 7. % Powerful Tools, IV: Metrics on measures 8. Rest of the Digression Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  3. This talk includes a survey 1975-present. Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  4. This talk includes a survey 1975-present. It is not and cannot be complete. Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  5. This talk includes a survey 1975-present. It is not and cannot be complete. Surveys are often left to OLD ... (oh, wait.) Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  6. This talk includes a survey 1975-present. It is not and cannot be complete. Surveys are often left to OLD ... (oh, wait.) Will spice it up by showing you some things that are cool (my opinion), have potential, and are not all widely known. Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  7. This talk includes a survey 1975-present. It is not and cannot be complete. Surveys are often left to OLD ... (oh, wait.) Will spice it up by showing you some things that are cool (my opinion), have potential, and are not all widely known. - potentials for interaction - velocity averaging - functionals - metrics on measures, with applications. Let’s begin! Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  8. Key Words & Themes BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  9. Key Words & Themes BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , DSMC and Relatives 3 , Qualitative Matters 4 , Related Equations (endless!) 5 , Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  10. Key Words & Themes BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , DSMC and Relatives 3 , Qualitative Matters 4 , Related Equations (endless!) 5 , Spatially Homogeneous Cases 6 , Soft potentials, and/or no angular cutoff 7 Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  11. Many (but not all) People BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , DSMC and Relatives 3 , Qualitative Matters 4 , Related Equations (endless!) 5 , Spatially Homogeneous Cases 6 , . . . Maxwell and Boltzmann (0,4); Hilbert, Chapman and Enskog (4); Grad (4); Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  12. Many (but not all) People BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , DSMC and Relatives 3 , Qualitative Matters 4 , Related Equations (endless!) 5 , Spatially Homogeneous Cases 6 , . . . Maxwell and Boltzmann (0,4); Hilbert, Chapman and Enskog (4); Grad (4); After 1972: Cercignani (0-6); Lanford, Spohn (0); Pulvirenti & I, Shinbrot & I, Arkeryd, Caflisch (0,1,2,3,4) Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  13. Many (but not all) People BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , DSMC and Relatives 3 , Qualitative Matters 4 , Related Equations (endless!) 5 , Spatially Homogeneous Cases 6 , . . . Maxwell and Boltzmann (0,4); Hilbert, Chapman and Enskog (4); Grad (4); After 1972: Cercignani (0-6); Lanford, Spohn (0); Pulvirenti & I, Shinbrot & I, Arkeryd, Caflisch (0,1,2,3,4) Bird, Nanbu, Babovsky & I, Frezzotti, Sone, Aoki (3, 4) Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  14. Many (but not all) People BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , DSMC and Relatives 3 , Qualitative Matters 4 , Related Equations (endless!) 5 , Spatially Homogeneous Cases 6 , . . . Maxwell and Boltzmann (0,4); Hilbert, Chapman and Enskog (4); Grad (4); After 1972: Cercignani (0-6); Lanford, Spohn (0); Pulvirenti & I, Shinbrot & I, Arkeryd, Caflisch (0,1,2,3,4) Bird, Nanbu, Babovsky & I, Frezzotti, Sone, Aoki (3, 4) Wagner, Rjasanow, Pareschi, Russo (3) Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  15. Many (but not all) People BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , DSMC and Relatives 3 , Qualitative Matters 4 , Related Equations (endless!) 5 , Spatially Homogeneous Cases 6 , . . . Maxwell and Boltzmann (0,4); Hilbert, Chapman and Enskog (4); Grad (4); After 1972: Cercignani (0-6); Lanford, Spohn (0); Pulvirenti & I, Shinbrot & I, Arkeryd, Caflisch (0,1,2,3,4) Bird, Nanbu, Babovsky & I, Frezzotti, Sone, Aoki (3, 4) Wagner, Rjasanow, Pareschi, Russo (3) Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  16. BE, Derivation and Validation 0 , Solvability 1 , Discrete Velocity Models 2 , DSMC and Relatives 3 , Qualitative Matters 4 , Related Equations (endless!) 5 , Spatially Homogeneous Cases 6 , Soft potentials, and/or no angular cutoff 7 Cabannes (2), Toscani (2,6), Boblylev (1,2,4,6), DiPerna, Lions (1), Golse, Perthame, Degond, Wennberg (1,2,4,5,6) Desvillettes, Villani, Carrillo (1,5,6) Levermore (1,4,5), Gamba (3,4,5,6), St. Raymond (4). Morimoto, Ukai, Yang (7). If I have not listed (forgotten) you or one of your friends, forgive me... Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  17. A List of Tools ◮ BBGKY & Boltzmann hierarchies (Bogolyubov, Cercignani, Lanford) ◮ Perturbation Series as solutions (control of the hierarchies) ◮ Free Flow domination for rare clouds (I, Shinbrot) ◮ Velocity Averaging & renormalization (DiPerna, Lions) ◮ Potentials for Interaction (Varadhan, Bony, Beale for DVMs) ◮ Regularization by the collision operator (Yang, Morimoto, Ukai) Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  18. Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  19. Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  20. Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  21. Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  22. Tools, I: Potentials for Interaction An Example: Dicrete Velocity Models in 1 Dimension Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  23. Tools, I: Potentials for Interaction An Example: Dicrete Velocity Models in 1 Dimension Equations: � A jk u i , t + c i u i , x = i u j u k =: F i j , k Potential for interaction gives uniform global control of � t � u i u j dx dt . This, combined with some other (older) tricks, 0 produces global uniform boundedness and the existence of wave operators (in the absence of boundaries). Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  24. Tools, I: Potentials for Interaction An Example: Dicrete Velocity Models in 1 Dimension Equations: � A jk u i , t + c i u i , x = i u j u k =: F i j , k Potential for interaction gives uniform global control of � t � u i u j dx dt . This, combined with some other (older) tricks, 0 produces global uniform boundedness and the existence of wave operators (in the absence of boundaries). All we need is � F i = 0 = � c i F i (mass and momentum conservation). Then the following fantastic calculation works: Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  25. Assume c i � = c j if i � = j . Let � � � I ( t ) = ( c i − c j ) u i ( x ) u j ( y ) dx dy . x < y y i , j Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  26. Assume c i � = c j if i � = j . Let � � � I ( t ) = ( c i − c j ) u i ( x ) u j ( y ) dx dy . x < y y i , j Note: I(t) is bounded by mass conservation! One computes � � dI � = ( c i − c j )[ F i ( y ) u j ( x ) + u i ( y ) F j ( x )] dx dy dt y x < y � �� � i , j sum to 0 , by conservations � � y + ( c i − c j )( − c i u i , x ) u j ( y ) dx dy −∞ � � ∞ + ( c i − c j ) u i ( x )( − c j u j , y ) dy dx x Do the inner integrals, collect terms.... Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

  27. So, � � � I ( t ) = ( c i − c j ) u i ( x ) u j ( y ) dx dy y x < y i , j gives � dI � ( c i − c j ) 2 u i ( x ) u j ( x ) dx , dt = − ij Reinhard Illner, Victoria A Selective “Modern” History of the Boltzmann and Related Equati

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